ScalingStacks

Example 3.28 . [03PL]

Original official author HTML, exact retained edition. Historical TeX conversion verdicts remain unchanged. Cited-edition alignment and mathematical self-containment are not assessed.

Complete original source context · Original author HTML

Example 3.28.

Let (M,J,g,Ω)(M,J,g,\Omega) be a Calabi–Yau mm-fold for m⩾2m\geqslant 2, LL a compact Lagrangian in MM, and p∈Lp\in L. In [57], Neves defines another Lagrangian L~\tilde{L} in MM, which is Hamiltonian isotopic to LL and coincides with LL except in a small open neighbourhood of pp. Here L,L~L,\tilde{L} are locally SO(m)\mathop{\rm SO}\nolimits(m) surfaces of revolution on the curves in sketched in Figure 3.7. (Actually Neves restricts to m=2m=2, but the same ideas should work for all m⩾2m\geqslant 2.)

∙\textstyle{\bullet}p\textstyle{p}∙\textstyle{\bullet}×\textstyle{\times}×\textstyle{\times}×\textstyle{\times}×\textstyle{\times}×\textstyle{\times}×\textstyle{\times}×\textstyle{\times}×\textstyle{\times}×\textstyle{\times}×\textstyle{\times}L\textstyle{L}L~\textstyle{\tilde{L}}

Figure 3.7: Neves’ Lagrangian with a finite time singularity under LMCF

Neves’ main result [57, Th. A] is that Lagrangian MCF starting from L~\tilde{L} develops finite time singularities. This is important, as it shows that finite time singularities in Lagrangian MCF are unavoidable in many situations (although note that L~\tilde{L} has phase variation greater than π\pi, so this does not show that almost calibrated Lagrangian MCF has finite time singularities).

LT1\textstyle{L^{T_{1}}}∙\textstyle{\bullet}∙\textstyle{\bullet}L1T1\textstyle{L^{T_{1}}_{1}}∙\textstyle{\bullet}L2T1\textstyle{L^{T_{1}}_{2}}=\textstyle{=}∐\textstyle{\amalg}

Figure 3.8: First singular time t=T1t=T_{1} of Lagrangian MCF from L~\tilde{L}

What actually happens in Lagrangian MCF starting from L~\tilde{L}? Neves’ proof does not tell us, as he assumes for a contradiction that no finite time singularity occurs. The author expects a Lagrangian MCF with surgeries {Lt:t∈[0,T)}\{L^{t}:t\in[0,T)\} in MM with L0=L~L^{0}=\tilde{L}, with two singular times 0<T1<T2<T0<T_{1}<T_{2}<T. For t∈[0,T1),t\in[0,T_{1}), LtL^{t} looks much like L~\tilde{L}, but as t→T1t\rightarrow T_{1} in [0,T1)[0,T_{1}), the region marked with crosses ‘×\times’ in Figure 3.7 undergoes a ‘neck pinch’. At t=T1t=T_{1}, as sketched in Figure 3.8, LT1L^{T_{1}} decomposes as L1T1∐L2T1L^{T_{1}}_{1}\amalg L^{T_{1}}_{2}, where L1T1L^{T_{1}}_{1} is a small immersed 𝒮m{\mathbin{\cal S}}^{m} near pp with one transverse self-intersection point with μL+,L−​(p)=m+1\mu_{L_{+},L_{-}}(p)=m+1, a ‘Whitney sphere’ as in Example 3.23, and L2T1L^{T_{1}}_{2} looks quite like the original LL.

Then as tt increases from T1T_{1} to T2T_{2}, the component L1tL^{t}_{1} should shrink to a point, until at the second singular time t=T2t=T_{2} it undergoes ‘collapsing a zero object’ as in Principle 3.25. Meanwhile, the Lagrangian MCF of L2tL^{t}_{2} looks quite like that of the original LL, and continues for t>T2t>T_{2}. Thus, at least conjecturally, Neves’ examples [57] are not counterexamples to the programme of §3.2.

Original mathematics by the credited authors. Source-backed reader collection; mathematical self-containment is not assessed.